Robin boundary condition

Robin boundary condition

In mathematics, the Robin (or third type) boundary condition is a type of boundary condition, named after Victor Gustave Robin (1855-1897) who lectured in mathematical physics at the Sorbonne in Paris and worked in the area of thermodynamics. [Gustafson, K., (1998). Domain Decomposition, Operator Trigonometry, Robin Condition, "Contemporary Mathematics", 218. 432-437.] When imposed on an ordinary or a partial differential equation, it is a specification of a linear combination of the "values" of a function and the values of its "derivative" on the boundary of the domain. "Robin" should be pronounced as a French name, although some English speaking mathematicians anglicize the word.

Robin boundary conditions are a weighted combination of Dirichlet boundary conditions and Neumann boundary conditions. This contrasts to mixed boundary conditions, which are boundary conditions of different types specified on different subsets of the boundary. Robin boundary conditions are also called impedance boundary conditions, from their application in electromagnetic problems.

If Omega, is the domain on which the given equation is to be solved and partial Omega denotes its boundary, the Robin boundary condition is

: a u + b frac{partial u}{partial n} =g on partial Omega,

for some non-zero constants a, and b, and a given function g, defined on partial Omega. Here, u, is the unknown solution defined on Omega,, and partial u/partial n denotes the normal derivative at the boundary. More generally, a, and b, are allowed to be (given) functions, rather than constants.

In one dimension, if, for example, Omega= [0, 1] ,, the Robin boundary condition becomes the conditions

:a u(0) - bu'(0) =g(0),:a u(1) + bu'(1) =g(1).,

(notice the change of sign in front of the term involving a derivative, that is because the normal to [0, 1] at 0 points in the negative direction, while at 1 it points in the positive direction).

Robin boundary conditions are commonly used in solving Sturm-Liouville problems which appear in many contexts in science and engineering.

In addition, the Robin boundary condition is a general form of the insulating boundary condition for convection-diffusion equations. Here, the convective and diffusive fluxes at the boundary sum to zero:

:-D frac{partial c(0)}{partial x}+ u_x(0),c(0)=0,

where "D" is the diffusive constant, "u" is the convective velocity at the boundary and "c" is the concentration. The first term is a result of Fick's law of diffusion.

ee also

*Dirichlet boundary condition
*Neumann boundary condition
*Mixed boundary condition
*Cauchy boundary condition

References


*Gustafson, K. and T. Abe, (1998a). (Victor) Gustave Robin: 1855–1897, "The Mathematical Intelligencer", 20, 47-53.

*Gustafson, K. and T. Abe, (1998b). The third boundary condition - was it Robin's?, "The Mathematical Intelligencer", 20, 63-71.

*cite book
last = Eriksson
first = K.
coauthors = Estep, D.; Johnson, C.
title = Applied mathematics, body and soul
publisher = Berlin; New York: Springer
date = 2004
pages =
isbn = 3540008896

*cite book
last = Atkinson
first = Kendall E.
coauthors = Han, Weimin
title = Theoretical numerical analysis: a functional analysis framework
publisher = New York: Springer
date = 2001
pages =
isbn = 0387951423

*cite book
last = Eriksson
first = K.
coauthors = Estep, D.; Hansbo, P.; Johnson, C.
title = Computational differential equations
publisher = Cambridge; New York: Cambridge University Press
date = 1996
pages =
isbn = 0521567386

*cite book
last = Mei
first = Zhen
title = Numerical bifurcation analysis for reaction-diffusion equations
publisher = Berlin; New York: Springer
date = 2000
pages =
isbn = 3540672966


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